2011
DOI: 10.1088/0957-4484/22/34/345703
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Theoretical characterization of the topology of connected carbon nanotubes in random networks

Abstract: In recent years, a lot of attention has been paid to carbon nanotube (CNT) networks and their applications to electronic devices. Many studies concentrate on the percolation threshold and the characterization of the conduction in such materials. Nevertheless, no theoretical study has yet attempted to characterize the CNT features inside finite size CNT networks. We present a theoretical approach based on geometrical and statistical considerations. We demonstrate the possibility of explicitly determining some r… Show more

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Cited by 24 publications
(22 citation statements)
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“…Numerous works have been devoted to the electrical and optical properties of transparent films with elongated fillers such as NTs, NWs, and nanorods. [3][4][5][6][7][8][9][10][11][12][13][14] However, the use of films containing conducting nanorings [15][16][17] looks extremely attractive since, in this case, there are no dead ends in the percolation cluster, i.e., the percolation cluster is identical to its geometrical backbone. In a two-dimensional continuum percolation, the number density is defined as where N is the number of objects randomly deposited onto a square substrate of size L×L with periodic boundary conditions (PBC).…”
Section: Introductionmentioning
confidence: 99%
“…Numerous works have been devoted to the electrical and optical properties of transparent films with elongated fillers such as NTs, NWs, and nanorods. [3][4][5][6][7][8][9][10][11][12][13][14] However, the use of films containing conducting nanorings [15][16][17] looks extremely attractive since, in this case, there are no dead ends in the percolation cluster, i.e., the percolation cluster is identical to its geometrical backbone. In a two-dimensional continuum percolation, the number density is defined as where N is the number of objects randomly deposited onto a square substrate of size L×L with periodic boundary conditions (PBC).…”
Section: Introductionmentioning
confidence: 99%
“…and the number of fibres per unit area will be ݊ , = ܰ ݊ ,,ଵ (16) Using (16) and (13) we can rewrite (15) as…”
Section: B Effect Of Contact Conductancementioning
confidence: 99%
“…The number of contacts per fibre predicted by the MCM for a 2D material with truncated Gaussian, non-uniform, angular distributions were compared with the value predicted by Heitz [16] for a uniform angular fibre distribution. For a uniform angular PDF, Heitz's theory fits closely to the MCM results, and for truncated Gaussian PDFs the number of contacts is reduced though it is still proportional to the fibre concentration.…”
Section: Effect Of Anisotropy On the Number Of Contacts Per Fibrementioning
confidence: 99%
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“…In Figure 5 we have also plotted the theory of where    p is the angular PDF for the fibres in the material which we have described in detail in [10] and  is the angle of the fibre in the xy-plane, relative to the x-axis. We also considered the average the number of contacts per fibre, which is predicted by Heitz et al [11] for the 2D isotropic case. .…”
Section: Figure 4 Effect Of 1 M Contact Resistance On Veil With Unimentioning
confidence: 99%